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QSO absorption spectra and -variation Group meeting 2 July 2007 Ruth Buning, Wim Ubachs, Michael Murphy, Lex Kaper, Huib Henrichs, Piet Mulders
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Has changed on a cosmological timescale?
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Empirical search for a change in Compare H 2 spectra of different epochs: Compare H 2 spectra of different epochs: QSO 12 Gyr ago Lab today 90-112 nm x (1+z)
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/ and spectrum H 2 Recent finding, based on 76 lines in 2 QSO absorbers: Recent finding, based on 76 lines in 2 QSO absorbers: Accurately calculated Lab: 5 x 10 -8 QSO: (2-10) x 10 -7 4σ4σ
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The QSO absorption sample >2300 HI absorption systems >2300 HI absorption systems ~600 DLA’s ~600 DLA’s 14 H 2 absorption systems (~15%) 14 H 2 absorption systems (~15%) 6 useful 6 useful 3 high-quality spectra 3 high-quality spectra Q0405: 37 lines at z abs =2.59 Q0405: 37 lines at z abs =2.59 Q0347: 39 lines at z abs =3.02 Q0347: 39 lines at z abs =3.02 J2123: ~50 lines at z abs =2.06 J2123: ~50 lines at z abs =2.06 1 next august 1 next august Q2348: ~20 lines at z abs =2.43 Q2348: ~20 lines at z abs =2.43
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Aug. ’07 observations: The Instrument
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Kueyen
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Aug. ’07 observations: The Instrument
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UVES: Ultraviolet – Visual Echelle Spectrograph
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300-500 nm 420-1100 nm
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Spectrum quality Resolving power R= Resolving power R= –slitwidth SNR SNR –brightness/sky background –seeing –airmass –total exposure time
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Aug. ’07 observations: Object data
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Blue CCD chip Red CCD chip 1Red CCD chip 2 Lyman- of quasar emission z emis =3.0236 C IV emission DLA at z abs =2.426 H 2 region z abs =2.426 DLA at z abs =2.615
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Blue CCD chip Red CCD chip 1Red CCD chip 2 Lyman- of quasar emission z emis =3.0236 C IV emission DLA at z abs =2.615 H 2 region z abs =2.426 DLA at z abs =2.93 DLA at z abs =2.426
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Spectrum Q2348 DLA at z abs =2.426 Strong Ly H 2 region Ly at z abs =2.615 Lyman limit at z abs =2.615
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Spectrum Q2348 DLA at z abs =2.615 DLA at z abs =2.426 H 2 region Ly at z abs =2.615 Lyman limit at z abs =2.93
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Data: H 2 absorption L0R0 line of H 2 > 7 velocity components
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Aug. ’07 observations: Spectrum quality Now: Now: –Total exposure time 4.5 hr –R = 47,000 –SNR = 15 August: August: –Total exposure time 22 hr –R = 55,000 –SNR = >35
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J2123 spectrum (Keck/HIRES, Prochaska) H 2 region Resolution 110,000 ; z abs =2.0593
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J2123 spectrum H2H2 Ly
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Spectrum analysis Voigt profile Voigt profile Input: Input: – i 0 –K i –Oscillator strengths Fit parameters: Fit parameters: –Column density –Doppler parameter –z abs – Also fit blended Ly forest lines Also fit blended Ly forest lines
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Summary: QSO data for / determination Q0347: 37 lines Q0347: 37 lines Q0405: 39 lines Q0405: 39 lines Q2348: ~20 lines -> Aug. ‘07 Q2348: ~20 lines -> Aug. ‘07 J2123: ~50 lines -> to be analyzed J2123: ~50 lines -> to be analyzed
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The QSO absorption sample Q 0515-441z=1.15 Q 1331+170z=1.78 Q 0551-336z=1.96 Q 0013-004z=1.97 Q 1444+014z=2.09 Q 1232+082z=2.34 Q 0841+129z=2.37 Q 2343+125z=2.43 Q 2348-011z=2.43 Q 0405-443z=2.59 Q 0528-250z=2.81 Q 0347-383z=3.02 Q 0000-263z=3.39 Q 1443+272z=4.22 …… Q 0515-441z=1.15 Q 1331+170z=1.78 Q 0551-336z=1.96 Q 0013-004z=1.97 J2123 z=2.06 Q 1444+014z=2.09 Q 1232+082z=2.34 Q 0841+129z=2.37 Q 2343+125z=2.43 Q 2348-011z=2.43 Q 0405-443z=2.59 Q 0528-250z=2.81 Q 0347-383z=3.02 Q 0000-263z=3.39 Q 1443+272z=4.22 …… H 2 very weak/tentative Too low z
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Energy levels in a diatomic molecule Electronic Electronic Vibrationalv Vibrationalv RotationalJ RotationalJ
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Representation of the energy levels Rotation: Rotation: Vibration: Vibration: (Rigid rotor) (Nonrigid rotor) (Harmonic oscillator) (Anharmonic oscillator)
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Dunham representation Energies derived from Schrödinger equation and general potential function Energies derived from Schrödinger equation and general potential function These contain the parameters e and B e, which are mass-dependent These contain the parameters e and B e, which are mass-dependent
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The sensitivity coefficients Dependence of transition wavelengths (or energies) on quantified by sensitivity coefficients: Dependence of transition wavelengths (or energies) on quantified by sensitivity coefficients: E and dE/dµ derived from Dunham expansion: E and dE/dµ derived from Dunham expansion:
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The H 2 data Available lab data: Available lab data: –Lyman (B-X): v’=0-18, v’’=0 –Werner (C-X): v’=0-4, v’’=0 –J between 0 and 5
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